Slide - The MESA Lab - University of California, Merced

advertisement
MESA LAB
On tempered and substantial fractional
calculus
YangQuan Chen
Collaborators: Jianxiong Cao, Changpin Li
School of Engineering,
University of California, Merced
Department of Mathematics, Shanghai University
E: yangquan. chen@ucmerced.edu
MESA LAB
Outline
• Preliminaries of fractional calculus
• Tempered and substantial fractional operators
• Numerical solution of a tempered diffusion
equation
• Conclusion
MESA LAB
Preliminaries
• Calculus=integration+differentiation
• Fractional Calculus= fractional integration+
fractional differentiation
• Fractional integral:
Mainly one: Riemann-Liouville integral
• Fractional derivatives
More than 6: not mutually equivalent
RL and Caputo derivatives are mostly used
MESA LAB
Preliminaries
• Left Riemann-Liouville integral
• Right Riemann-Liouville Integral
• Left Riemann-Liouville fractional derivative
• Right Riemann-liouville Fractional derivative
MESA LAB
• Left Caputo fractional derivative
• Right Caputo fractional derivative
• Riesz fractional derivative
• Riesz-Caputo fractional derivative
where
MESA LAB
Slide-6/1024
Tempered and substantial operator
Let
be piecewise continuous on
integrable on any subinterval of
,and
,
1) The left Riemann-Liouville tempered fractional
integral is
2) The right Riemann-Liouville tempered fractional
integral
Slide-7/1024
MESA LAB
(Phys. Rev. E 76, 041105, 2007 )
Suppose that
be
times continuously differentiable on
,
and times derivatives be integrable on any subinterval
of
, then the left and right Riemann-Liouville tempered
derivative are defined
and
Slide-8/1024
MESA LAB
Remark I: From the above definitions, we can see if
then they reduce to left and right Riemann-Liouville
Fractional derivatives.
Remark II: The variants of the left and right Riemann-Liouville
tempered fractional derivatives (Boris Baeumer, JCAM, 2010)
Slide-9/1024
MESA LAB
(Phys. Rev. Lett. 96, 230601, 2006)
Substantial fractional operators
Let
be piecewise continuous on
, and integrable on
any subinterval of
, then the substantial fractional
integral is defined by
And the substantial derivative is defined as
where
Slide-10/1024
MESA LAB
Theorem:
If the parameter
is a positive constant, the tempered
and substantial operators are equivalent.
See our paper for the details of proof.
Recently, tempered fractional calculus is introduced in
Mark M. Meerschaert et al. JCP(2014).
Slide-11/1024
MESA LAB
Numerical computation of a tempered diffusion
equation
We consider the following tempered diffusion
equation
where
Slide-12/1024
MESA LAB
The exact solution of above problem is
We use finite difference method and shifted Grunwald
method to numerically solve it, we choose different value
Of parameter
, and compare the results with its exact
solution
Slide-13/1024
MESA LAB
Slide-14/1024
MESA LAB
Slide-15/1024
MESA LAB
Slide-16/1024
MESA LAB
 From the figures, we can see that the
numerical solution are in good accordance
with exact solutions.
 It is easily shown that the peak of the
solutions of tempered diffusion equation
becomes more and more smooth as
exponential factor λ increases.
MESA LAB
Conclusion
• Tempered and substantial fractional calculus are
the generalizations of fractional calculus.
• The two fractional operators are equivalent,
although they are introdued from different
physical backgrounds.
• Tempered fractional operators are the best tool for
truncated exponential power law description
MESA LAB
Thanks for your attention
Download